ASDEX Upgrade Team’s research while affiliated with Max Planck Institute for Plasma Physics and other places

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Publications (629)


Integrated Data Analysis and Validation
  • Preprint

November 2024

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6 Reads

R. Fischer

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A. Bock

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ASDEX Upgrade Team

A major challenge in nuclear fusion research is the coherent combination of data from heterogeneous diagnostics and modelling codes for machine control and safety as well as physics studies. Measured data from different diagnostics often provide information about the same subset of physical parameters. Additionally, information provided by some diagnostics might be needed for the analysis of other diagnostics. A joint analysis of complementary and redundant data allows, e.g., to improve the reliability of parameter estimation, to increase the spatial and temporal resolution of profiles, to obtain synergistic effects, to consider diagnostics interdependencies and to find and resolve data inconsistencies. Physics-based modelling and parameter relationships provide additional information improving the treatment of ill-posed inversion problems. A coherent combination of all kind of available information within a probabilistic framework allows for improved data analysis results. The concept of Integrated Data Analysis (IDA) in the framework of Bayesian probability theory is outlined and contrasted with conventional data analysis. Components of the probabilistic approach are summarized and specific ingredients beneficial for data analysis at fusion devices are discussed.


Designing a Validation Experiment for Radio Frequency Condensation
  • Preprint
  • File available

October 2024

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33 Reads

Theoretical studies have suggested that nonlinear effects can lead to "radio frequency condensation", which coalesces RF power deposition and driven current near the center of a magnetic island. It is predicted that an initially broad current profile can coalesce in islands when they reach sufficient width, providing automatic stabilization. Experimental validation of the theory has thus far been lacking. This paper proposes experiments on DIII-D for testing and refining the theory of the nonlinear effects.

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FIG. 1. Histogram comparing the distribution of values of both actuators and profiles used in this study for DIII-D (blue) vs AUG (orange). Note that the primary statistical difference is the size of the devices, the toroidal field, the gas and density, and the shaping. For reference, the q 0 = 1 surface and the I p < 0.9MA and 1.0MA < I p < 1.2MA regions are shown on the corresponding plots.
FIG. 3. Via curriculum learning, the model can be tuned to arbitrary number of timesteps. Here are shown models optimized for a single timestep (20ms, in red), which has lower error σ at 20ms (red dashed line), and 10 timesteps (200ms, in blue), which has lower error at later times (blue dashed line). For reference, error for predictions where profiles are assumed to stay constant at the initial values is also plotted, in black.
FIG. 4. Typical loss curve for curriculum learning. For the first 250 epochs teacher forcing is used, and the model need only predict one timestep (20ms) ahead. The model then begins randomly using its own output autoregressively as input for predicting the next timestep, with an increasing probability of autoregression (i.e. average number of steps per autoregressive rollout) between epoch 250 and 750 from 20ms up to 200ms. Between epoch 750 and the end of training a probability corresponding to an average number of steps of 200ms is used.
FIG. 5. Comparing σ error (Equation 1) with AUG database with and without normalization, along with bleeding AUG data into DIII-D data.
FIG. 9. In concatenated context learning, the in-distribution dataset (in this case I p 0 to 0.9MA) is used to train a data-driven model, with additional inputs from simulations. The network is tested outof-distribution (I p from 1.0 to 1.2MA), again with the added context from simulations.

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Combing physics-based and data-driven predictions for quantitatively accurate models that extrapolate well; with application to DIII-D, AUG, and ITER tokamak fusion reactors

September 2024

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26 Reads

Methodologies for combining the accuracy of data-driven models with extrapolability of physics-based models are described and tested, for the task of building transport models of tokamak fusion reactors that extrapolate well to new operational regimes. Information from multiple physics simulations (the ASTRA transport code with gyro-Bohm and TGLF estimates for turbulent diffusion) as well as multiple distinct experiments (DIII-D and AUG tokamaks) are considered. Applications of the methodology to the task of commissioning and controlling a new reactor such as ITER are discussed.


Tomographic reconstructions of the fast-ion phase space using imaging neutral particle analyser measurements

April 2024

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29 Reads

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6 Citations

In this paper we demonstrate how the inversion, in energy and major radius (E, R) coordinates, of imaging neutral particle analyser (INPA) measurements can be used to obtain the fast-ion distribution. The INPA is most sensitive to passing ions with energies in the range (20-150) keV and pitches near 0.5 in the core and 0.7 near the plasma edge. Inversion of synthetic signals, via 0th -order Tikhonov and Elastic Net regularization, were performed to demonstrate the capability of recovering the ground truth fast-ion 2D phase-space distri- bution resolved in major radius and energy, even in the presence of moderate noise levels (10%). Finally, we apply our method to measure the 2D phase-space distribution in an MHD quiescent plasma at ASDEX Upgrade and find good agreement with the neoclassical fast-ion distribution predicted by TRANSP.


Commissioning of the Imaging Neutral Particle Analyzer for the ASDEX Upgrade tokamak

January 2024

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28 Reads

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7 Citations

An Imaging Neutral Particle Analyser (INPA) diagnostic has been installed and commissioned at the ASDEX Upgrade (AUG) tokamak. The AUG INPA diagnostic provides energy and radially resolved measurements of the fast-ion (FI) distribution, complementing the existing set of diagnostic which measure the confined FI population. To this end, it analyses charge exchange (CX) neutrals produced in reactions between FI and neutrals injected by a neutral beam injector. These CX neutrals are ionized by a 20 nm carbon foil and deflected towards a scintillator by the machine magnetic field. The use of a scintillator as active component allows us to cover the whole plasma radial range with an energy resolution of 9 keV and a spatial of 7 cm for 93 keV deuterons. First measurements demonstrate the high sensitivity of the INPA diagnostic to different AUG fast-ion distribution functions, from NBI and ion-cyclotron resonance heating (ICRH) origin, and show good agreement with the synthetic diagnostic.



On learning latent dynamics of the AUG plasma state

August 2023

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24 Reads

In this work, we demonstrate the utility of state representation learning applied to modeling the time evolution of electron density and temperature profiles at ASDEX-Upgrade (AUG). The proposed model is a deep neural network which learns to map the high dimensional profile observations to a lower dimensional state. The mapped states, alongside the original profile's corresponding machine parameters are used to learn a forward model to propagate the state in time. We show that this approach is able to predict AUG discharges using only a selected set of machine parameters. The state is then further conditioned to encode information about the confinement regime, which yields a simple baseline linear classifier, while still retaining the information needed to predict the evolution of profiles. We then discuss the potential use cases and limitations of state representation learning algorithms applied to fusion devices.



Targeting a Versatile Actuator for EU-DEMO: Real Time Monitoring of Pellet Delivery to Facilitate Burn Control

May 2023

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22 Reads

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2 Citations

Fusion Science & Technology

Core particle fueling, an essential task in the European demonstration fusion power plant EU-DEMO, relies on adequate pellet injection. However, pellets are fragile objects, and their delivery efficiency can hardly be assumed to be unity. Exploring kinetic control of the EU-DEMO1 scenario indicates that such missed-out pellets do cause a considerable problem for keeping a burning plasma. Missed-out pellets can cause a severe drop of plasma density that in turn results in a potential drastic loss of burn power. Efforts are under way at the ASDEX Upgrade (AUG) tokamak aiming to provide real-time monitoring of pellet arrival and announcement of missed-out cases to the control systems. To further optimize the controllers, system identification experiments have been performed to identify the dynamic response of the system to the actuators.


MHD simulations of formation, sustainment and loss of Quiescent H-mode in the all-tungsten ASDEX Upgrade

January 2023

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55 Reads

Periodic edge localized modes (ELMs) are the non-linear consequences of pressure-gradient-driven ballooning modes and current-driven peeling modes becoming unstable in the pedestal region of high confinement fusion plasmas. In future tokamaks like ITER, large ELMs are foreseen to severely affect the lifetime of wall components as they transiently deposit large amounts of heat onto a narrow region at the divertor targets. Several strategies exist for avoidance, suppression, or mitigation of these instabilities, such as the naturally ELM-free quiescent H-mode (QH-mode). In the present article, an ASDEX Upgrade equilibrium that features a QH-mode is investigated through non-linear extended MHD simulations covering the dynamics over tens of milliseconds. The equilibrium is close to the ideal peeling limit and non-linearly develops saturated modes at the edge of the plasma. A dominant toroidal mode number of n=1 is found, for which the characteristic features of the edge harmonic oscillation are recovered. The saturated modes contribute to heat and particle transport preventing pedestal build-up to the ELM triggering threshold. The non-linear dynamics of the mode, in particular its interaction with the evolution of the edge safety factor is studied, which suggest a possible new saturation mechanism for the QH-mode. The simulations show good qualitative and quantitative agreement to experiments in AUG. In particular, the processes leading to the termination of QH-mode above a density threshold is studied, which results in the transition into an ELM regime. In the vicinity of this threshold, limit cycle oscillations are observed.


Citations (53)


... Equation (1) can be discretized [33] (S = WF where all additional factors (e.g. phase-space volume elements) have been absorbed in W) and established tomographic inversion methods [8,14,15,25,29,34,35,[37][38][39][40][41][42][43] can then be used to reconstruct the fast-ion distribution from measurements. To be able to use equation (1) as is, we require that s bt ≫ s tt (2) s bt ≫ s bb (3) where s bt is the signal component originating from reactions between fast ions and thermal ions (so-called beam-target), s tt is the signal component originating from reactions amongst thermal ions, and s bb is the signal component originating from reactions amongst fast ions. ...

Reference:

Reconstruction of the fast-ion deuterium distribution in a tritium-rich plasma in the JET DTE2 campaign
Tomographic reconstructions of the fast-ion phase space using imaging neutral particle analyser measurements

... This section outlines the operational principles of FILDs and INPAs and introduces the mathematical framework used to obtain the fast-ion velocity distribution from their measurements. Detailed descriptions are documented in [33][34][35][36][37][38]. ...

Commissioning of the Imaging Neutral Particle Analyzer for the ASDEX Upgrade tokamak

... A total of 12 W-coated (thickness ~ 400 nm) graphite marker samples, embedded in a custom W-target tile, were prepared for exposure with DIM-II. The second tile on the DIM-II probe head was equipped with bulk W samples with pre-exposure fuzz and nanoscale features created in the PSI-2 linear plasma device and a set of polished W samples; the analyses of these samples are discussed elsewhere [16,17]. Each marker sample had a surface area of 33.5 × 12 mm 2 with either three 1 × 1 mm 2 or two 5 × 5 mm 2 evenly spaced Pt spots (thickness 40-50 nm) deposited on the W layer in a magnetron sputtering device. ...

FIB line marking as a tool for local erosion/deposition/fuzz formation measurements in ASDEX Upgrade during the He campaign
  • Citing Article
  • October 2023

Nuclear Materials and Energy

... The auxiliary gas puff is reduced while pellets are injected to avoid an excessive total fuel flux, which could potentially lead to an edge density limit and confinement degradation. The neutral density in the divertor is used as a suitable measure of the edge density, even when pellets are injected [45]. Figure 1 shows the time evolution of a discharge in which pellets drive the core electron density, while reducing of the gas puff rate compensates for the increased particle flux from pellet injection and stabilizes the neutral density level in the divertor. ...

Targeting a Versatile Actuator for EU-DEMO: Real Time Monitoring of Pellet Delivery to Facilitate Burn Control
  • Citing Article
  • May 2023

Fusion Science & Technology

... To get further confidence that the observed structures in T e originate from magnetic islands, we utilized the resistive MHD code called JOREK 42 . JOREK modelling of ASDEX-Upgrade experiments with RMPs 43 has made advances allowing the calculation of the plasma response to the RMP field with realistic viscosity, with free boundary 44 and realistic anisotropy between parallel and perpendicular electron heat transport. ...

Non-linear free boundary simulations of the plasma response to resonant magnetic perturbations in ASDEX Upgrade plasmas

Journal of Physics Conference Series

... This level of accuracy assumes a filterbank-like acquisition system, and is sufficient to relate any observed variations in P fus to those in T i and to monitor anomalous ion heat transport from the core. In addition, it enables tracking the impact on T i of core fuelling with the proposed DEMO pellet launching system [45] on timescales below the anticipated maximum pellet delivery rate of ≳10 Hz. Furthermore, the accuracy on T i estimated here can be readily improved with longer integration times and/or by replacing the filter bank with a high frequency resolution fast digitizer, as discussed in section 3.2. ...

Concept for a multi-purpose EU-DEMO pellet launching system
  • Citing Article
  • December 2022

Fusion Engineering and Design

... This pitch profile, calculated for discharge #41090, can be seen in figure 1, together with the fast-ion distribution calculated with the TRANSP code [35]. Full details of the diagnostic design, installation, validation and instrument functions can be found at [29,30,36,37]. ...

Imaging Neutral Particle Analyzer Engineering Design and Installation for the ASDEX Upgrade Tokamak
  • Citing Article
  • November 2022

IEEE Transactions on Plasma Science

... An example is inferring electron density and temperature profiles by combining a Thomson scattering and interferometers [29,30]. Hence, the GPR has been adopted for profile fittings by many research groups including JET [29,[31][32][33], Alcator C-Mod [34,35], ASDEX-U [36], W7-X [37,38], LHD [30], and KSTAR [4]. Furthermore, Gaussian process (GP) itself has been used for other research topics such as correcting faulty magnetic pickup probes [39], suppressing quasi-coherent noise [40] and the noise modeling [41]. ...

Gaussian Process Tomography at ASDEX Upgrade with Magnetic Equilibrium Information and Nonstationary Kernels

Fusion Science & Technology

... The ICRF electrostatic wave is first produced by a generator called a tetrode, which is essentially a multistage amplifier of the power composed of a cascade of electron tubes. Each stage of which increases the power by approximately an order of magnitude, from watts to megawatts [1]. ...

The prospects of ICRF generators at ASDEX upgrade
  • Citing Article
  • September 2020

AIP Conference Proceedings